Phase indicator



April 13, 1943. E. M. IRWIN 21,316,434

PHASE INDICATOR Original Filed Aug. l2, 1940 3 Sheets-Sheet l April 13, 1943. E M, lRWlN PHASE 'INDICATOR Original Filed Aug. l2, 1940 5 Sheets-Sheet 2 IOIIO 0 I April 13 1943- a M. IRWIN 2,316,434

PHASE INDICATOR.

Original Filed Aug. l2, 1940 3 Sheets-Sheet 3 Patented Apr. 13, 1943 PHASE INDICATOR EmmettM. Irwin, Longr Beach, Calif., assigner to Magnetest Corporation, Long Beach, Calif., a corporation of California Original application August 12, 1940, Serial No.

Divided and this application March 11, 1941, serial No. ssasss 14 Claims.

This application is a division of my application Serial No. 352,280 tiled August 12, 1940, entitled Method of and apparatus for testing properties of materials.

My invention relates to a phase indicator, of a type which is particularly useful in connection with the electrical testing of the properties of materials.

It has been proposed, heretofore, to test the properties of materials, such as magnetic materials for example, by utilizing the material to be tested to ailect a circuit excited by an alternating current, and observing the effect of the material upon the electrical characteristics of the alternating current circuit or electrically related circuit, to determine the presence of defects or the physical properties of the material. In this manner materials have been tested to determine defects in the material such as cracks, surface irregularities, internal flaws, blowholes, pipes resulting from inclusions of slag in rolling down the material from an ingot, and also to determine the effect of heat treatment, hardness, chemical composition, and magnetic properties. These tests generally have been made by referring the observed magnitudes to a known standard by comparing the effect on the alternating current circuit of a standard specimen of known properties with the effect of a specimen of unknown properties to be tested, or by simultaneous effects of the standard and the specimen to be tested on related alternating current circuits.

Unless the phase relation of the voltage and the current in the alternating current circuit affected by the material is determined, the results observed in these tests may be very misleading. A small magnitude of voltage or current may be indicated, when in fact; the .magnitude is large, because the measurement of the magnitude may be made in such phase relati'on as to give only a small magnitude, which is merely a component part of the true larger magnitude. Furthermore, there is a relationship between the phase angle of the voltage and the current in the alternating current circuit and the properties of the material being tested, so that one may measure the magnitude of an electrical characteristic of the alternating current ycircuit with the impressicn that the magnitude represents a condition or property of the material, whereas in fact if the phase relation were known it would indicate that the magnitude represented a different property than the one under consideration.

In some tests of this kind determinations have been made of the phase relation between the voltage and the current in an alternating current circuit affected by the material tested. However, the determinations have been made by constructing the phase relation from observed data. By this procedure it is diillcult to accurately relate the measurements of phase angle and amplitude, which results in erroneous observations. Furthermore this procedure is almost impossible to carry out effectively if the material being tested is being moved with respect to the alternating current circuit, as is required in testing rods, pipes, or other long pieces of material, because the changes in phase ordinarily would occur too rapidly to permit such observations. The failure to observe these rapid phase changes has lead to erroneous results.

An object of my invention is to provide an improved arrangement for indicating or recording a magnitude functionally related to the phase angle between the voltage and the current in the alternating current circuit affected by the material to be tested. I accomplish this by providing an amplifier without variable phase distortion for amplifying the relatively feeble voltage or current observed in the alternating current circuit and indicating or recording the output from the amplifier in terms of phase angle.

Another object of my invention is to provide an improved phase indicator for alternating current circuits.

Further objects and advantages of my invention will be apparent as the following description proceeds, and the features of novelty which characterize my invention will be pointed out with particularity in the claims annexed to and forming a part of this specification.

In the drawings, Fig. 1 is a schematic diagram of an apparatus for electrically testing materials, and embodying the constructional features of my novel phase indicator; Fig. 2 is a diagrammatic illustration of the electron discharge circuits employed in connection with my improved phase indicator or recorder; Fig. 3 is a diagram illustrating certain electrical characteristics of the circuits shown in Fig. 2; Fig. 4 is a front elevation of my improved phase indicator or recorder and amplitude indicator and recorder; Fig. 5 is a front view of a portion of a record sheet or chart obtained in the operation of the indicator or recorder shown in Fig. 4; Fig. 6 is a sectional view on the line B--G of Fig. 4; Fig. 7 is a diagrammatic view of the construction shown in Fig. 6 illustrating how one of the styluses is moved out of recording position with respect to the record sheet when the other stylus is moved into recording position with respect thereto: Pig. 8 is a detailed view of the joint between the ends of the steel ribbon which I preferably employ as the endless band of the recorder on which the styluses are mounted; Fig. 9 is an enlarged cross sectionalview of one of the styluses or pens employed on the band of the phase recorder; Fig. l is an enlarged sectional view on line Il-il of Fig. 6. showing the manner of mounting the rollers for supporting the band.

Referring to the drawings, in Fig. l I have shown schematically an entire electrical testing system embodying the novel features of my improved phase indicator or recorder. The elec, trical testing system illustrated is for the purpose of testing properties of materials. In this system a specimen it of magnetizable material. such as a sucker rod from an oil well, a drill pipe used in drilling oil wells, or other suitable bar, is supported on rollers I and I2. so as to be movable longitudinally. In order to move the specimen il as desired, it may be moved on the rollers by hand, or by a driving motor Il, which keeps the specimen It within the desired range of speed of movement. The specimen I0 is moved coaxially through primary windings I4 and il arranged on opposite sides of a secondary winding i6. The windings |4 and It are wound in the same direction, so as to give'an additive effect to their ampere turns. The windings i4, Il, and il are supported in coaxial relation with the specimen it in any suitable manner, and provide for free movement of the specimen through the coils. The windings i4 and Il are connected in series at and across an alternating current source of supply Il. I have found it to be satisfactory to utilize the alternating current source of supply Il at nity cycle frequency, and a current filter Ila is provided in the circuit to pass to the coils i4 and I5 only a pure sine wave current of fifty cycle frequency. The secondary winding I8 is preferably placed in the center of the space between the windings i4 and il. The secondary winding Il is connected by conductors Ila and lib to a fifty cycle band pass filter I9, passing any frequency, which it is desired to study as modied by the changes in the characteristics of the specimen Il. The band pass filter I! is connected by conductors 2l to a voltage amplifier 2|. The voltage amplifier 2|, if desired, may be a current amplifier, so long as the output therefrom through conductors 22 to a stationary solenoid 22 of a recorder 24 is a function of an electrical characteristic of the secondary circuit associated with the secondary coil i8.

The construction of the recorder 24 is clearly shown in Figs. 1, 4, 6, 7, 8, 9, and l0. In order to record an amplitude functionally related to an electrical characteristic of the secondary circuit associated with the secondary coil It, the recorder 24 is provided with a stylus or pen 2l mounted on the lower end of arm 2l, which is pivotally supported on the body of the recorder at 21. The horizontal arm 2t is rigidly attached to the ver tical arm 26 of the recorder, and the outer end of the arm 2l is pivotally connected at 29 to a soft iron armature 30 suspended within the stationary solenoid 23. The arms 2l and 2l are balanced by a spring 28a, and a stop 26a limits the range oi movement of the arm 20. A record of the magnitude to be indicated by the stylus 25 on the record member or chart 3| is obtained by maintaining the record sheet in a stretched condition in cooperative relation with the stylus 2l and close to the opening 22 in the front of the recorder. I provide an upper roller 2l upon which the record sheet is wound, and a lower roller 24 from which the record sheet is wound. the rollers ll and 24 being supported in suitable bearings. The edges of the record sheet prefer ably are perforated at Ila along the edges to prevent slipping by engagement with suitable teeth associated with the rollers 23 and 34. The rollers 2l and I4 are geared together by an arrangement including a slip clutch or belt. so that upon driving the rollers Il and 24 to move the record sheet as indicated by the arrow Il, the record sheet is maintained in a taut condition. I have found it convenient to make the scale of the record sheet, or chart, so that one-tenth of an inch of movement of the chart indicates one foot of movement of the specimen Il. The roller I3 is, therefore, connected to a driving shaft ll through suitable reduction gearing. l

The shaft Il is driven in timed relation to the movement of the specimen Il by connecting the roller I2 to the rotatable element of a dynamoelectric machine or self synchronous motor l1 by a flexible shaft Il. The shaft Il is connected to the rotatable element of the dynamo-electric machine'll, which is provided with a two pola concentrated winding, the winding being connected through suitable brushes to conductors Il. The dynamo-electric machine Il also has a three phase distributed winding which is connected to a three phase alternating current source of supply 4|.

The conductors Il are connected to the winding of a rotatable member of a dynamo-electric machine or self synchronous motor 42, which is like the dynamo-electric machine l1. This rotatable member has a two pole concentrated winding connected with the conductors Il by suitable brushes. The stationary member of the dynamo-electric machine 42 has a three phase distributed type winding connected by the conductors 4I to the three phase alternating current source of supply 4I. By this arrangement of the dynamo-electric machines 31 and 42, movement of the specimen Il is transmitted through the roller I2. flexible shaft Il, and machines 31 and 42 to the shaft Il, and the chart Il is moved as indicated by the arrow Ii in the desired timed relation to the movement of the test specimen il.

In order to obtain the most sensitive relation ship between the specimen Il to be tested and the secondary coil It. I prefer to introduce a balancing wave in the secondary circuit associated with the coil It. This balancing wave, or opposing electrical characteristic, is in the present arrangement fifty-cycle pure sine wave, so as to be the same as the alternating current source oi supply il exciting the coils i4 and I l. The bal ancing wave should balance out the component of the frequency of the fimdamental or harmonic. which it is desired to study as affected by the specimen il. This balancing wave may be equal and opposed to an electrical characteristic of the secondary circuit of the ooil Il, such as the voltage, or it may be made slightly less for convenience in obtaining a reference for measurement and comparison. The particular manner of utilizing this balancing wave or electrical characteristic in making the electrical test will be more fully hereinafter explained, but the purpose is to `establish electrical relations in the electrical testing system most favorable for the observation or recording of results.

This balancing wave is introduced into the cir cuit by providing a non-inductive resistor 44 in".

. characteristics above fifty cycles from the winding 46 to the resistor 44. The lters 48 and I8 should be changed in accordance with the component of frequency required in the particular test. A switch 5Ia is provided to connect and disconnect the winding 46 from the resistor 44, as desired. The phase shifting transformer 41 is provided with a three phase distributed windv` ing, which is connected at 58 to a three phase alternating current source of supply, the frequency of the source of supply of 53 being fifty cycles to correspond with the frequency of the alternating current source of supply I8, or other frequency relating the particular characteristic of the specimen I being investigated. A dial 45h is provided for adjusting the position of the concentrated winding 46 on the rotatable member of the phase shifting transformer 41, a scale being provided to indicate three hundred and sixty electrical degrees corresponding to one complete revolution of the rotatable member 46. This arrangement provides for interposing into the secondary circuit associated with the coil I6 a single phase pure sine wave alternating current of fifty cycle frequency, the phase relation of which can be varied as desired by the rotation of a rotatable member 46, and the magnitude of which can be varied by an adjustment of the slider I on the variable resistor 50.

Delicate measurements of the relations of the voltage, or other electrical characteristic, in the secondary circuit associated with the ccil I8, may be made by a dynamometer D having a field core 54 and a two pole concentrated winding or armature 55 mounted on a suitable core and rotatably supported adjacent the end of the field core 54. The armature core and winding 55 are connected at 56 to an indicating hand 51, which in the de-energized condition of the dynamometer remains in a zero position on a scale 51a, but may move in either direction to indicate the voltages in opposite directions. The field core 54 of the dynamometer is provided with a field exciting winding 58. This field exciting winding 58 is connected across a concentrated two pole winding 59 of a vphase shifting transformer 60 through suitable brushes 59a to provide for rotation of the rotatable member carrying the winding 59. A filter 6I is arranged in the cir cuit to filter out all frequencies above fifty cycles, so that the field exciting winding 58 of the dynamometer is excited by a single phase fifty cycle pure sine wave alternating source of supply. The stationary member of the dynamo-electric machine 60 is provided with a three phase dis tributed winding connected to an alternating current source of supply 62, which is in the .present arrangement fifty cycles but should correspond to the frequency of the balancing wave. The rotatable member of the dynamo-electric machine 68 is also provided with a dial 59h indicating three hundred and sixty electrical degrees for one complete revolution. By rotation of the rotatable member carrying the winding 58 the phase relation of the voltage and the current supplied to the field exciting winding 58 of the dynamometer D can be varied as desired. The movable coil or armature of the dynamometer is connected to the poles 88 of a two pole two position switch, shown in its open position. When` the poles 88 of the switch are closed in their upper position the armature 55 'is connected across the conductors I1 and I8, so as to be connected across the secondary circuit associated with` the coil I4. In their lower closed position the poles 58 of the switch connect the armature 55 of the dynamometer, through conductors 84, across a noninductlve resistor 85, which is connected in series with the terminal of the winding I5 connected to the alternating current source of supply I8.

For convenience in measurement, I lprefer to relate the phase relation of an electrical characteristic of the secondary circuit, and an electrical characteristic of the balancing wave introduced intothe secondary circuit by the phase shifting transformer 41 through the resistor 44, to the current in the alternating current source of supply I8. I do this by closing the poles 88 of the switch to their lower position to connect the armature 55 of the dynamometer D across the resistor 65. The position of the rotatable member 58 of the phase shifting transformer 60 is then adjusted until the dynaimometer indicator 51` reads zero, and the angular position of the rotatable member 59a is noted. This indicates that the single phase in the field exciting winding 58 of the dynamometer is in quadrature phase relation to the alternating current source of supply I8. I then close the poles 53 of the two positlon switch in their upper lposition to connect the armature 55 of the dynamometer D across the second-ary circuit I1 and I8. The rotatable member 59 of the phase shifting transformer 68 is then adjusted until the dynamometer reads zero.` 'I'his indicates that the fifty cycle voltage supplied from the rotatably adjustable winding 58 is in quadrature phase relation to the voltage of the secondary circuit connected to the secondary coil I6. The phase shifting transformer 41 is now put in circuit by closing the switch 5Ia and the rotatable member 46 is also adjusted until the dynamometer D reads zero, which indicates that the single phase fifty cycle voltage supplied from the winding 46 is -also in quadrature with the voltage in the secondary circuit I1 and I8. The voltage of the balancing wave introduced at 44 now may be in phase with the voltage and current in the secondary circuit I1 and I8, or one hundred and eighty degrees out of phase. If the voltage of the balancing wave introduced at 44 is in opposition to the secondary voltage, the dynamometer D may be adjusted to zero by adjustment of the slider 5I of the variable resistor 58. If it is found that the voltage of the balancing Wave introduced at 44 and the secondary voltage are not in opposition, it will be necessary merely to rotate the adjustable winding 46 one hundred and eighty electrical degrees and then adjust dynamometer D to zero. In measuring the characteristics of some materials having very widely varying characteristics it may be desirable not to balance the voltage in the secondary circuit I1 and I8 to zero with the balancing wave interposed at 44, but provide for a slight unbalance by making the balancing wave slightly less than the voltage in the secondary circuit.

After the balancing wave is introduced through the resistor 4I into the secondary circuit associated with the coil Il, as above described. the specimen il is moved through the coils Il. Il, and I3. The variations in the properties of the specimen l will affect the amplitude and phase in the secondary circuit in accordance with the characteristics of the material. and the magnitude of the relative changes will be indicated by the stylus or pen 2t, which is controlled by the solenoid 23, receiving energy from the secondary circuit through the filter Il. The chart or record sheet 3| will be moved by the dynamo-electric machines 31 and l2, in accordance with the movement of the specimen I 0, as indicated by the arrow 3l in Fig. l. This will cause the stylus 2l to trace a curve il on the record sheet. Unless the phase relation of the voltage and current in the alternating current circuit affected by the specimen I0 is determined, it is impossible to correctly interpret the significance of the magnitude changes indicated at t6 on the record sheet, which are magnitudes functionally related to the voltage or electrical characteristic of the alterhating current circuit affected by the specimen. I, therefore, provide an arrangement for independently and simultaneously indicating or recording a magnitude functionally related to the phase relation between the alternating voltage and the alternating current in the alternating current circuit associated with the coil I3, which are affected in magnitude and phase by the specimen |0 excited from the alternating current source of supply i3.

This indication of phase angle is preferably recorded separately from the indication of magnitude shown by the curve It, but is recorded in timed relation to the indication of magnitude given by the curve Si, and in timed relation to the movement of the specimen I0. 'I'he phase relations are, therefore, preferably recorded at l1 on the record sheet 3| with ordinates extending horizontally, so that every magnitude variation of the curve 6B is coordinated in relation to the magnitude related to the phase relations indicated by the curve 61. Such a record sheet is shown in Fig. 5. The curve 61 is traced on the record sheet 3| by a stylus or pen il, as clearly shown in Fig. 6. The stylus 83 is mounted on its endless band 69, which is supported in iront of the record sheet 3| in the form of an elongated loop by a plurality of rollers. Two of these rollers 10 and 1| rotate about vertical axes and are mounted on a body member or plate 12 rigidly supported on the body of the recorder. The spacing of the axes of the rollers 1|) and 1| is such as to provide for an indication of a phase angle variation of three hundred and sixty electrical degrees upon movement of the pen I3 from one extreme of its range of movement to the other extreme of its range of movement. The endless band E9 is also supported on another larger pulley or roller 13. which is` mounted so as to rotate about a vertical axis by being rigidly attached to a vertical shaft 1l. The shaft 1l connects together the rotatable members of the two vertically arranged dynamo-electric machines or self synchronous motors 15 and 13. The endless band B9 is retained under tension by an idler pulley arrangement including a pulley 11 pivotally secured at 1l to a movable arm 13. The arm 19 is pivoted at 8l to the supporting member 12, and an arm Il beneath the supporting member 12 is rigidly connected to the arm 1s. The arm 8| is acted upon by a tension spring l2 attached at 83 to the supporting member 12.

The idler pulley 11 is thus acted upon by the spring l2 with sufficient force to maintain the desired tension in the band N. 'Ihe necessary movement of the roller 11 is obtained by extending the pivotal support 13 through an elongated arcuate slot Il in the plate 12. The particular manner oi mounting the rollers or pulleys 1l, 1|, and 11 on their supports to provide for free rotation is shown in Fig. l0. A spindle 35 is threaded into the body oi' the supporting member 12. The spindle Il is provided with a shoulder I3 secured in engagement with the supporting member 12. and the lower end of the roller 10 is recessed to receive the shoulder, and provide clearance between the bottom of the roller 1I and the supporting member 12. The roller 10 is removably secured to the spindle Il by a round plate 31 secured to the top of the spindle Il by a machine screw 33. 'I'he rollers 10 and 1| are secured to the supporting member 12 in the same manner, and the idler pulley or roller 11 is secured to the outer end of the arm 1! in a similar manner.

The endless band is preferably made of a thin ribbon of steel Joined together at the opposite ends, as shown in Fig. 8. The ends of the ribbon are cut oi! at an angle at a and rounded at 83h. One end is provided with a bayonet slot having a restricted portion llc and an enlarged portion 39d. 'I'he ends are overlapped to cover the bayonet slot, and the other end has a pin "e rigidly attached thereto. The pin 38e closely flts the restricted portion 33e of the bayonet slot, and is provided with an enlarged head tightly nlttting against the side of the ribbon about the s o The styluses il, 03a, "b, and c are all of the same construction. Any suitable form of stylus may be employed to produce the curves 33 and 31 on the record sheet 3|. I prefer. however, to utilize a pen type stylus having an ink well provided with a fine point extending in engagement with the record sheet. This construction is shown in Fig. 9. The pen I3 includes a cylindrical body extending vertically the width of the endless band 69. The body is provided with an ink well 83a open at the top for convenience in filling, and a sharp pointed stylus 63h having a passage c therein extending from the ink well 33a to the sharp point "d oi' the stylus. The body of the ink well is attached to a flange Ole extending the width of the band I3, and is secured thereto by rivets ill, it being understood that the flange portion e of the stylus may be secured to the band 3l in any other suitable manner.

The endless band Il is retained in driving engagement with the pulley 13 mounted on the shaft of the dynamo-electric machine 13, by the spring-pressed idler pulley 11. The portion oi the band is between rollers 1|) and 1| also will be retained under tension. If the recorder is sub- Jected to vibration the band 39 may vibrate and cause irregular marking on the record sheet 3|, and also spilling ink from the well 88a. I suppress these undesirable vibrations by providing supports 12a and 12b arranged between the rollers 1|| and 1|l and 10 and 13 respectively. These supports have a rounded face engaging the band and extending the entire width thereof, and are secured at their lower ends by screws 12o and 12d respectively to the supporting member 12. The supporting member 12 is secured to the upper end-shield of the lower dynamo-electric machine 18 by suitable screws, and the dynamo-elecl tric machines or self synchronous motors 15 and f with respect to the other one.

2 3 16,434 16 are secured to the body of the recorder by bolts extending through the feet. The shafts o! these dynamo-electric machines are arranged in vertical alignment, and connected together at 16a by a coupling provided with set screws, which rigidly attach the shafts and rotatable -members of the machines together. The dynamo-electric machines or seli' synchronous motors 15 and 16 are normally maintained energized and produce torque in opposite directions, the torque of one machine being balanced to produce equilibrium An arrangement is provided for actuating one or the other of the machines, so that the angular movement of the machine corresponds to'variations in phase relation, thus providing an angular measurement of the changes in phase. The dynamo-electric machines and 16 constitute polyphaseelectrical elements in equilibrium, or electrical translating devices.

In the particular construction illustrated, one complete rotation of the machines 15 and 16, in response to phase variations, is equal to three hundred and sixty electrical degrees. The pulley 13, therefore, is made of such circumference that one rotation thereof by the dynamo-electric machines 15 and 16, in recording variations in phase, equals three hundred and sixty electrical degrees, This causes the pen 68 to traverse the entire distance between the rollers 10 and 1i, the direction of movement of the pen 68 depending upon the direction of the shift of phase. 'I'he pen 68 is shown in zero degree phase positionA in Fig. 6 of the drawings. If the shift in phase is more than ninety degrees to the right as shown in Fig. 6, the pen 68 will pass over the roller 1| passing through the position shown in Fig. 7 of the drawings. When the pen 68 moves into this position shown in Fig. '1, the pen 68a moves into the position shown, so that for a phase shift in this direction of ninety degrees the pen 68 will record the variation. On the other hand if the pen 68 undergoes a phase variation indication greater than ninety degrees, it will move around the pulley 1| out of recording relation to the record sheet 3|. However during this movement, the pen 68a will continue to indicate the recorded range of phase variation at the other side of the chart or record sheet. If the change in phase occurs in the other direction, then the pen 68a will move out of engagement with the record sheet 3|, and the pen 68 will move into engagement therewith. 'I'he pens 68, 68a, 68h, and 68e, are all equally spaced apart, so that whatever range of movement may occur in the rotation of the pulley 13, at least one of the pens 68, 68a, 68h, or 68e, will be in recording relation to the record sheet 3|. It will thus be seen that one of these pens records one range of recorded variation, whereas the other pen records another range of recorded variation. Since the record sheet 3| is driven in accordance with the range of movement of the material, or specimen 0, the record of variations in phase indicated by the curve 61, and the record indicated by the curve 66 of the variations in amplitude will remain in timed relation to each other, and in timed relation to the movement of the material to be tested.

In order to record the changes in phase in the secondary circuit associated with the secondary coil I6, I provide an amplifier for phase measurement 88, which receives energy through conductors 89 and the fifty cycle band pass filter I9 from the secondary circuit associated with the secondary coil I6. The energy received by the ampliiier 88 is widely variable due to the changes caused by the specimen I8 in the electrical characteristics of the secondary circuit associated with the secondary coil I6. I, therefore, construct the amplier 88 so that it has no variable phase distortion. Whatever phase changes occur in passing through the amplifier 88, the changes are constant without regard to the widely variable input from the band pass filter I9. The dynamoelectric machines 15 and 16 are thus actuated to give a true indication of phase, without effects of variable distortion. The stationary member of the dynamo-electric machine 15 is provided with a three phase distributed winding connected to a suitable alternating current source of supply by the terminals 82, and the dynamo-electric machine 16 is also provided with a three phase distributed winding connected to a suitable alternating current source of supply through the terminals 93. The rotatable members of the dynamo-electric machines 15 and 16 are mounted in suitable bearings, and each is provided with a concentrated two pole winding connected through suitable brushes to the conductors 90 and 9| respectively.

The torques produced by the rotatable members of the dynamo-electric machines 15 and 16 are opposed and equal, and as they are connected by the coupling 16a they are in equilibrium. The torque produced by each of these dynamo-electric machines is in two components. One component is due to the ilux induced in the core of the rotatable member bythe three phase rotating iield. In some machines this component may be small, in others it may be large, due to the particular design. The other component of the torque is produced by the single phase current induced to iiow in the concentrated two pole winding |20 or |22 of the rotatable members when these windings supply current to an external load. If the stationary members are excited from a three phase source of supply and the windings |20 or |22 of the rotatable members are connected to a load the rotatable members tend to operate as in a motor. The input to the winding of the rotatable member of the dynamo-electric machine 15 through the conductors 90 causes the same to assume a position due to the concentrated two pole winding, which is a direct measurement of the phaserelation of the voltage and current supplied to the rotatable member through the conductors 90. .This is caused by the rotating field of the stationary member acting upon the nux produced by the single phase excitation of the winding of the rotatable member to a position of Azero current in the winding. For this reason, three hundred and sixty degrees of rotation of the dynamo-electric machine 15 under the action of the winding of the rotatable member is equal to three hundred and sixty electrical degrees. If the concentrated two pole windings of the rotatable members of the dynamo-electric machines 15 and 16 are made four pole, or any even multiple of two pole, the degree of rotation of the shafts 14 indicating three hundred and sixty electrical degrees will be something less than three hundred and sixty mechanical degrees, which is well understood in the art. If a greater number of poles were used the pulley 13 would be correspondingly changed in size, so that the pens 68, shown in Fig. 6 and in Fig. 7, would `be actuated to move three hundred and sixty electrical degrees in accordance with three hundred and sixty electrical degrees of movement of the rotatable members of the dynamo-electric machines 1I and 1I.

Under low, or zero, input to the amplifier for phase measurement Il the two pole concentrated winding of the rotatable member of the dynamoelectric machine 1l will be loaded by the amplifier et, so that energy flows from the two pole winding to the amplifier. 'I'his tends to cause rotation of this dynamo-electric machine. Under this condition the machines are exactly balanced in equilibrium by supplying energy from the two pole concentrated winding of the rotatable member of the dynamo-electric machine 18 through the conductors 8 This particular mode of operation and construction will be more fully understood by reference to the diagrammatic illustration of Fig. 2 to be hereinafter more fully described, in which the amplifier for phase measurement 88 includes all of the circuits between the tube 9B and the leads l0 and II connected to the output of the transformers Il! and |45 respectively.

As pointed out in discussing the construction of Fig. 1, the energy received by thevamplifier for phase measurement Il through conductors Il and the fifty cycle band pass filter I9 from the secondary circuit associated with the coil It is of a very low magnitude, and widely variable, due to the variations produced by the characteristics of the specimen I in passing through the coils I4, I5, and I8. The amplifier 88 has such charaoteristics that the widely variable low power input thereto is highly amplined to give suflicient power to actuate the dynamo-electric machines and 16, as required to record the variations in phase. This amplification is effected without any variable phase distortion between the voltage and the current from the input to the output of the amplifier 88. The output from the amplifier ll is constant and whatever phase changes may occur within the amplifier 88 are constant throughout the range of low variable energy input thereto. so that the phase recorded by the curve i1 on the chart 3| is not affected by the widely varying character of the input to the amplifier 88. The particular manner of obtaining these characteristics are more fully explained hereinafter with reference to Fig. 3.

The electron discharge circuit arrangements employed in the amplifier are shown schematically in Fig. 2. The tubes employed in the circuit arrangements may be of any suitable electron discharge type. The cathodes may be ither directly or indirectly heated in any suitable manner. The manner of heating the cathodes in the tubes illustrated in the drawings is not shown, in order to simplify the illustration in the drawings. The energy supplied to the amplifier I8 passes through several stages of amplification, the nrst stage being an amplifying tube 06. This amplifying tube 86 is resistance coupled to the succeeding amplifying tube by an arrangement including a plate circuit load resistor U1 connected to the plate 0l of the tube, a biasing resistor i! being provided for the cathode III! of the tube to control the voltage of the cathode within the desired range of variation. A by-pass condenser lla is provided around the resistor t! for the alternating current component of the plate circuit. The output from the tube l! is resistancecoupled to the succeeding amplifying tube III through resistors |02 and Ill, a blocking condenser IM for the direct current plate voltage applied to the tube Il, a variable resistor IIil, and

fying tube III.

aslider I" tothe grid |01 of thetube III. The 75 variable resistor Ill is provided for the WIPO of controlling the amplification of the tube and the succeeding stages of amplification. The blocking condenser I provides for the free iiow of the alternating current from the plate Il of the amplifying tube l0 to the grid Il1 of ampli- The cathode I of the amplifying tube IUI is provided with a biasing resistor Ill to control the voltage of the cathode. This resistor III is by-passed by a condenser Ill, so that the resistor will not interfere with the iiow of alternating current in the plate circuit of amplifying tube III. The amplified output of the tube I 0| is supplied through a push-pull type amplifying arrangement including an iron core transformer having its primary IIIa connected to the plate |I2 of the tube III. 'I'he secondary |||b of this transformer is connected to grids ||2 of amplifying tubes III, and the mid point of the secondary I||b is connected to -C battery. The cathodes of the tubes ||I are connected together at III and grounded at III. The plates ||1 of the tubes III are connected across the primary III of an iron core transformer I Il, and the mid point of the primary I I8 is connected to a +B battery. The secondary of the transformer II is connected across a two pole concentrated winding |20 of the dynamoelectric machine 1I through conductors n and suitable brushes of the machine. The secondary of the transformer III is tapped to provide for matching the impedance of the plate circuit of the tubes ||3. By this arrangement, the amplii'ied output from the tube lli through the transformer tubes IIS, and transformer Il! is supplied to the two pole concentrated winding |20 of the dynamo-electric machine 1I.

The stationary member of the dynamo-electric machine or self synchronous motor 1l is provided with a three phase distributed winding connected to a fifty cycle alternating current source of supply |2I, which is also connected to the three phase distributed winding of the stationary member of the dynamo-electric machine or self synchronous motor 1l. The output from the transformer I I8 excites the two pole concentrated winding |20 of the rotatable member of the dynamo-electric machine 15, and causes the rotatable member to move into a position angularly which is proportional to the angular phase relation between the voltage and the current in the circuit 00 supplying the alternating current to the winding |2I|. Under this condition, there is no energy output from the two pole concentrated winding of the rotatable member of the dynamoelectric machine 16, and the rotatable members of the dynamo-electric machines 1I and 1| are exerting opposing torque and in equilibrium throughout the range of angular movement required to record the variations in phase by movement of the shaft 14 and the pulley 1I, which drives the endless band I9 of the recorder. The dynamo-electric machine 1l does not have any output of energy from the rotatable two pole concentrated winding |22, because the grids III are biased beyond cut-off as will be hereinafter more fully explained.

In order to obtain substantially constant power output for actuating the dynamo-electric machine 1! in recording phase, I provide an arrangement in the amplifying electron discharge circuits between the input Il and the output Il of the ampliner il, which diverts energy from the amplifying circuit in direct prportion to the increase in energy, and conversely decreases the diversion of energy in the same proportion as the input decreases. This is done by providing an electron discharge circuit including two tubes |23 having their plates |24 connected at the opposite sides of the resistor |03, and their cathodes |26 grounded at |26 through a battery 21, the positive side thereof being connected to the cathodes. The number of tubes |23 may be varied as required to obtain the required load capacity and range of voltage variation. Under the conditions of low energy input the grids |26a of the tubes I 23 are biased beyond cut-oil` by the battery 21, as the grids |26a are then at ground potential, so that no energy is diverted from the amplifying circuit through the tubes |23. Upon increase of input to the amplifier the -grids |26a of the tubes |23 have their bias voltage raised in direct proportion to the increased input, so as to divert energy from the amplifying circuit through the tubes |23 by way of the plates |24 and cathodes |25. The voltage of the battery |21 is selected to cause the grids |26a of tubes |23 to begin diverting energy at X in the curves shown in Fig. 3. The tubes |23 thus serve as variable resistors to the flow of energy through the tubes by way of their plate circuits. The constant output at 90 from the amplifier 88 is indicated by the curve 90a in Fig. 3, and the energy diverted through the tubes |23 in proportion to the increased input to maintain constant output is indicated by the dotted curve |23a in Fig. 3. I

The necessary control of the grids 26a to obtain this result is obtained by making a connection at |21a lbetween. the plate 98 of the amplifying tube 96 and the resistor |02which is connected to ground through a blocking condenser |280, for blocking the plate voltage on the plate 98, and permitting the desired alternating current to pass therethrough, and through a resistor |28 having a slide |29 connected to the grid |30 of an amplifying tube |3|. By making the connection at |21a the tendency for the increased input to overload the amplifying tube |3| is avoided, because the increased input is immediately diverted through the tubes |23. The slider |29 controls the amplification in the tube |3|. 4'Ihe plate |32 of the tube |3| has a plate circuit load resistor |33 connected between the plate |32 and the +B battery. The output from the tube |3| is through a blocking condenser |34, to prevent the flow of B battery current through the succeeding tubes, but providing for the flow of the desired alternating current. The cathode |35 of the tube |3| is provided with a biasing resistor |36, which is provided with a by-pass condenser |31 connected across the same, so as not to interfere with theA flow of alternating current in the plate circuit of the tube. 'Ihe output from the amphfying tube |3| is to the plate |39 of a rectifying tube |38 having a plate loading resistor |40, which is grounded. .The cathode |4| of the rectifying tube |38 is grounded through a biasing resistor |42, and a by-pass condenser |43 for alternating current or undesirable pulsations. The upper end of the biasing resistor |42 is positive and connected to the grids |26a of the tubes |23 through a resistor |44. This resistor or choke |44 .must be made suiciently large to prevent any feedback through the tubes |23 to the input of the amplifying tube |3|, and also to suppress any undesirable ripples in the voltage on the grids |26a. Alternating current or pulsations are further carried from the grids |26a to ground through by-pass condenser. |44a. Such ripples or pulsations wouldbe reected into the amplifying circuits and interfere with the smooth operation of the amplifier in the operation of the phase recorder. By this arrangement the energy derived from the output of the amplifying tube 96, through the amplifying tube |3|, and the rectifying tube |38 controls the voltage on the grids I26a of the tubes |23, so as to divert energy from the amplifying circuit, as indicated by the dotted line |23a in Fig. 3, thus maintaining constant output from the ampliner 88.

lIn the amplier 88 shown in Fig. ,2, the resistors and the tubes may be selected to meet any particular requirements of design. However, if the values are chosen so that the resistors |02 and |03 each have one'unit of resistance, the resistor A |05 has ve units of resistance, and the tubes |23 are biased beyond cut-off to provide iniinite resistance, the output of the tube 96 is divided across seven units of resistance, the impedance of v the condenser |04 being negligible as compared to the values of the resistors, then the input to tube |0| would be 5/7 of the output of tube 96.

At the maximum grid bias the direct current plate resistance of each of the tubes |23 was chosen, so that the alternating current output from the plate of the tube 96 was divided across the resistor |02 and the plate resistance of the tube |23 to give approximately 1A, of the output of the tube 96 at the point |21a. The alternating current voltage at the plate of the second tube |23, or the input to' the tube |0| was approximately 1/5 of the output ofthe tube 96. If a third tube |23 were added then the input to the tube 10i would be approximately A25 of the output of the tube 96. then the input to the tube 0| would be approximately 1%525 of the output of the tube 96.

It will thus be seen that: two tubes |23 afford a Voltage ratio of 5/7 to Q5 or about 18 to 1; three tubes |23 afford a, voltage ratio of 5/1 to 1/125 or about 89 to 1; and four tubes afford a voltage ratio of 5/1 to $625 or about 446 to l. The number of tubes may be varied to obtain any desired variation.

I have obtained an even greater range of voltage variation by doubling the values of the resistors |02, |03, and |05. Under this condition when the tubes |23 are biased beyond cut-off to provide infinite resistance, the output of the tube 96 was divided across the resistors so that the input to the tube I0| was 5/1 of the output of the tube 96. At maximum bias of the tubes |23-the alternating current voltage was divided so that: the voltage at the plate of the first tube |23 was about t of the output of the tube 96; the voltage at the platel of the second tube |23 or the input to the tube 0| was about 1/{11 of the output of the tube 96; the voltage at the plate of a third tube |23, if added, would be about 1,629 of the output of tube 96; and-the voltage at the plate of a fourth tube |23, if added,.would be %5e1 of theV output of the tube 96. With this doubling of resistors |02, 03, and |05 the range of voltage variation afforded by the tubes |23 is as follows: two tubes about 58 to 1; three tubes about 520 to l; and four tubes about 4685 to 1.

When the input to the amplifier 88 decreases to a small value, somewhere between 0 andV X, as indicated in Fig. 3, the tubes ||3 provide a load for the two pole concentrated winding |20 of the lrotatable member of the dynamo-electric machine 15. As the stationary winding of the dynamo-electricmachine 15 is of the three phase distributed type, this loading of the two pole If a fourth tube were added .tubes |22.

concentrated winding |22 tends to cause the same to operate as a motor. In order to oppose the rotatable member of the dynamo-electric machine 15, to maintain ithe same in equilibrium under these conditions, the two pole concentrated winding |22 of the rotatable member of the dynamo-electric machine 12 is loaded by an amplifying and rectifying tube arrangement now to be described, so as to balance the torque exerted by the dynamoelectric machine 12. Ihe two pole concentrated winding |22 of the dynamof electric machine 12 is connected by conductors 2| and a variable resistor 2Ia across the secondary of the iron core transformer |45. The primary of this transformer is connected to plates |42 of amplifying tubes |41, the cathodes |42 of these tubes being connected together at |42 and grounded at |52. The mid point of the primary of transformer |45 is connected to +B battery. The grids |I of the tubes |41 are connected together at |52, a by-pass condenser |52 being provided to by-pass to ground any undesirable pulsations'or alternating current. Under this condition of zero or low input the tubes |41 load the two pole concentrated winding |22 of the dynamo-electric machine 12, so that the dynamo-eleotric machines and 12 are opposed in torque and in equilibrium. The grids I5| of the tubes |41 are at zero bias. so that they do not interfere with the flow of current Vthrough the tubes. As soon as the power input to the amplifier 22 increases it is apparent that there will be a reversed now of current in the output leads 22, so that energy will be supplied from the tubes |'I2 through the transformer |I2 to the two pole concentrated winding |22 of the dynamo-electric machine 15. The grids |2| of the tubes |41 then must be immediately biased beyond cut-off, so as to cut ofi th'e flow of current in the plate circuit through the primary of the transformer |42. When this pccurs the winding |22 of the dynamoelectric machine 12 is no longer loaded through the tubes/u1.

This rapid response is obtained by making a connection at |54 in the plate circuit of the tube |22 and between the resistors |22 and |22. Thus the increased input causes a flow of energy through the conductor |55, and blocking condenser I52 for the direct plate current of the The alternating current is impressed on the grid |51 of the amplifying tube |52 through a slider |52 of a variable resistor |22 connected between the condenser |52 and ground. The slider |52 provides for control of the amplification of the tube |52. The tube |52 is provided with a cathode |2I, a biasing resistor |22, and a by-pass condenser |62 connected thereto. The output of the amplifying tube |52 is through a plate circuit loading resistor |24 connected to the plate |55 of the tube. The plate |25 of the tube |52 is connected to an output circuit through a blocking condenser |22 for the direct current plate voltage, but which passes the desired alternating current to the cathode |21 of a rectifying tube |22. The cathode |21 has a biasing resistor |22 connected between the cathode and ground. The plate |12 of the tube |22 is connected to an output circuit including a loading resistor |1| and a by-pass condenser |12 for bypassing any undesirable pulsations or alternating current. The output of the plate circuit of the rectifying tube |22 is connected to the grids I2| of the tubes |41 through a resistor |12. By this arrangement, as soon as the input to the ampliiier 22 increases the energy is supplied through 75 the conductor |52 to the amplifying tube |22 the rectifying tube |22, so as to immediately supply a voltage through the resistor |12 to the grids |2I and bias the tubes |41 beyond cut-off, thus immediately preventing any further loading of the two pole concentrated winding. |22 of the dyna moelectric machine 12 by the tubes |41. IUnder this condition the-dynamo-electric machine 12 will be actuated to asume an angular position depending upon the phase relation of the voltage and the current supplied from the transformer I|2 through the conductors 22 to thevtwo pole concentrated winding |22. y

The'characteristics of operation of this amplitier will be clear from a consideration of the curve shown in Pig. 3.'- At zero load the plate current of the tubes |41 is indicated by OW. During the incremental increase of initial input 0 to X, the plate current of the tubes |41 is reduced to nero,

as indicated by the dotted curve |41a. DuringV this interval the output of the amplifier is increased gradually as indicated by the line OY, and then becomes constant throughout the further range of increase as indicated at 22d by the lineYZ. Atthepointxitwillbenotedthat the curve I22a is zero, but it increases in direct proportion to the input, which indicates that the energy diverted from the'ampllfier 22 through the tubes |22 keeps the output constant. It is to be understood, of course, that these curves represent the relation without taking into eect distortion, but this may be minimized by proper desian.

The operation of the foregoing construction and the particular method employed in the operation of the system will be clear from the foregoing description. however, the entire operation now will be briefly described. The specimen I2 may be any suitable length of material the characteristics of which are to be determined. These characteristics lmay be determined by carrying out and recording the test of the specimen and then comparing the curves obtained in the recorder 24 with the known standard properties. or another specimen the properties of which have been previously determined by testing the system. Preparatory to making the test, the specimen |2 isextended through the primary exciting coils I4 and I2 and the secondary coil I2, and a balancing wave of suitable magnitude is introduced into the secondary circuits I1 and I2 across the non-inductive resistor 44. In making the test the specimen I2 issupported on the rollers and |2 in coaxial relation with the exciting coils |4, I5, and the secondary coil I2. and the specimen is moved through the coils either manually, or by the driving arrangement indicated at I2, at a uniform speed suitable for the making of the test. The variations in the properties or characteristics of the specimen I2 affect the secondary coil I2 and the secondary circuits l1 and I2 associated therewith, and these effects are utilized to determine the characteristics of the specimen I2. A magnitude functionally related to an electrical characteristic of the secondary circuits I1 and I2 affected by the characteristics of the specimen I2 is recorded by supplying energy from the fifty cycle band pass filter i2 through conductors 22 to a voltage amplifier 2|, and energy is supplied from the voltage amplifier 2| through conductors 22 to a stationary solenoid 22 of the recorder 24. Thus the armature 22 is acted upon by the solenoid 22. so as to actuate the arm 22 and cause the stylus 25 to make a record of amplitude on therecord sheet 2| in coordinated or timed relation with the movement of the specimen, which operates the record sheet 3| through the roller i2 in contact with the specimen, flexible shaft 38. dynamo-electric machines 31 and 42 and the shaft 3l. By this arrangement, the amplitude variation shown by the curve It is a record o! a magnitude functionally related to theelectrical characteristic of the secondary circuit i1 and .I8 associated with the secondary coil I0, which is aiiected by the characteristics of the specimen Il excited by the primary coils i4 and Ii from the alternating current source of supply il. A

As previously explained, unless the curve of magnitude 86 indicated on the record sheet 3i is related also to the phase relation oi' the voltage and the current in the secondary circuit Il and Il associated with the secondary roll Il, the observed results may be very misleading. because phase relation and magnitude must be coordinately taken into consideration to determine the properties oi the specimen I0. Variations in phase are shown by the curve B1. which is traced on the moving chart Il by pen or stylus Il, as clearly shown in Figs. 1, 4, and 6. The styluses 08, Ola, Olb, andy c carried by the endless band BS-are controlled. so as to obtain the desired indication of variations in phase by the dynamo-electric machinesor self synchronous motors 15 and 18, which are in opposed torque relation and in equilibrium throughout their range of movement. Under low input to the amplifier 8l the dynamoelectric machine I is loaded by the ampliier 88 through the conductors lli, so that it tends to operate as a motor. This is opposed and balanced to a condition of equilibrium by the action oi' the dynamo-electric machine 1I, which is similarly loaded through the conductors 9| from the arnplier 8l, as explained in connection with the description oi' the construction and operation of the amplier 88 shown in Fig. 2. Beyond a low incremental input to the ampliiier 88 the dynamo-electric machine 1I is no longer loaded by the ampliiler 88 through the conductors 9|, because the grids I ll of tubes H1 are biased beyond cut-oil'. Under this condition the dynamo-electric machines 15 and I8 are producing opposed torque in equilibrium, and the dynamo-electric machine, 'i5 is actuated to its angular position in accordance with variations in phase. This causes the pulley i3 to operate the band $9 and one or more of the styluses 68, 88a, 68h, or 68e trace the curve oi phase variation as indicatedl at 67 in Figs. 1 and 5.

It will thus be seen that I have provided an improved phase indicator or recorder which is oi' particular utility in connection with a method and apparatus for electrically testing material by causing the material to aiect electrical characteristics of an alternating current circuit, which in this instance are recorded in timed relation to each other and in timed relation to the movement of the material being tested.

I do not desire my invention to be limited to the particular construction described, and I intend in the appended claims to cover all modiiications, which do not depart from the spirit and scope of my invention.

What I claim as new and Letters Patent of the United States, is:

l. A phase indicator adapted to receive low desire to secure by l and widely variable energy from an alternating current circuit and including an electrically responsive movable indicating means, means including an amplifier operable by low and widely variable energy input from the alternating current circuit tor a substantially constant energy output over the range of widely variable low input. and means responsive to the output of said ampliiler and actuating said movable indicating means i'or indicating the phase relation between the voltage and the current in the alternating current circuit supplying energy to said ampliiler.

2. A phase indicator for alternating current circuits including an electrical translating device, means includingan amplifier balancing the efiect oi said electrical translating device under minimum input to said amplifier and electrical translating device ior indicating the phase relation between the voltage and the current in an alternating current circuit. and means for rendering said ampliiler ineilective upon increased input to said ampliiier and during measurement of phase of the increased input.

3.A A phase indicator for alternating current ycircuits including an electrical machine, a second electrical machine connected to said first mentioned electrical machine and balancing the torque of the same throughout their range of movement, and means actuating said electrical machines for indicating the phase relation between the alternating voltage and the alternating current in an alternating current circuit.

4. A phase indicator tor-alternating current circuits including an electrically responsive movable indicating means, means including an electron discharge circuit for amplifying without variable phase distortion the input thereto from an alternating current circuit, and means responsive to said electron discharge circuit for actuating said movable said indicating means to indicate the phase relation in the alternating current circuit.

5. A phase indicator `for alternating current circuits including an electrically responsive movable indicating means, means including an electron discharge circuit for amplifying the input thereto, means responsive to said electron discharge circuit for actuating said movable indicating means to indicate the phase relations in an alternating current circuit above a minimum input to said ampliiler, and means for balancing said movable member during minimum input to said indicator.

6. A phase indicator for alternating current circuits including an electrically responsive movable indicating means, means including an elect and providing constant output without variabledistortion of the phase relation of voltage and current between the input and the output including an amplifier, means responsive to the output of said ampliiler for indicating the phase relation. of voltage and current in an alternating current circuit supplying energy to the input of said amplier. an electron discharge device, means including' a circuit from said ampliiier and the plate circuit through said electron discharge device for diverting energy from the output of said amplifier, and means varying theresistance of the plate circuit through said ampliiler inversely with respect to the input to said ampliiier for maintaining substantially constant output from said amplifier.

8. A phase indicator for alternating current circuits including a polyphase element arranged to produce torque in one direction, and means including a second polyphase element arranged to produce torque in balanced opposition to said iirst mentioned polyphase element for indicating the phase relation between the voltage and the current in an alternating current circuit.

9. A phase indicator for alternating current circuits including a polyphase sel! synchronous motor having stationary and rotatable members, means including a winding for exciting one of said members from a polyphase alternating current source of supply, means including a second winding associated with the other of said members for actuating the other of said members to an angular position related to the phase relation of the voltage and the current supplied from an alternating current circuit to said second winding, and means for balancing the component of torque of said other member due to the induced magnetic effect of said polyphase winding.

10. A phase indicator for alternating current circuits including a polyphase self synchronous motor having stationary and rotatable members, means including a winding for exciting one of said members from a polyphase alternating current source of supply, means including a second winding associated with the other of said members for actuating the other of said members to an angular position related to the phase relation of the valtage and the current supplied from an alternating current circuit to said second winding, and means including a second alternating current motor for balancing the component of torque of said other member due to the induced magnetic effect of said polyphase winding.

11. A phase indicator for alternating current circuits including a polyphase element arranged to produce torque in one direction, means including a second polyphase element arranged to produce torque in balanced opposition to said first mentioned polyphase element for indicating the phase relation between the voltage and the current in an alternating current circuit, and means for controlling the torque relation between said polyphase elements to obtain a balanced relation.

12. A phase indicator for alternating current circuits including a polyphase element arranged to produce torque in one direction, means including a second polyphase element for producing torque in balanced opposition to said first mentioned polyphase element, and means associated with one oi said polyphase elements and actuating said balanced elements for indicatin the phase relation between the voltage and current in an alternating current circuit.

13. A phase indicator adapted to receive low and widely variable energy from an alternating current circuit and including an electrically responsive movable indicating means. means including an ampliiler operable by low and widely variable energy input for maintaining substantially constant energy output and substantially constant phase angle relationship between the input and the output over a range oi widely variable low input, and means responsive to the output ot said ampliiler and actuating said movable indicating means for indicating the phase relation between the voltage and current in an alternating current circuit supplying energy to the input of said ampliiier.

14. A phase indicator adapted to receive low and widely variable energy from an alternating current circuit and including an electrically responsive movable indicating means, means including an ampliiier operable by low and widely variable energy input for maintaining substantially constant energy output and substantially constant phase angle relationship between the input and the output over a range of widely variable low input, said amplifier including a circuit for diverting energy from the output in the same proportion as the input increases, and means responsive to the output or said amplier and actuating said movable indicating means for indicating the phase relation between the voltage and current in an alternating current circuit supplying energy to the input of said amplifier.

EMIWE'I'I M. IRWIN. 

